Anthony
Griffiths
a,
Sarah L.
Boyall
a,
Pia
Müller
a,
John P.
Harrington
b,
Anna M.
Sobolewska
c,
William R.
Reynolds
c,
Richard A.
Bourne
ad,
Kejun
Wu
ef,
Sean M.
Collins
d,
Mark
Muldowney
c and
Thomas W.
Chamberlain
*a
aInstitute of Process Research and Development, School of Chemistry, University of Leeds, Leeds, UK. E-mail: t.w.chamberlain@leeds.ac.uk
bLeeds Electron Microscopy and Spectroscopy Centre, LEMAS, Bragg Centre for Materials Research, University of Leeds, Leeds, LS2 9JT, UK
cSterling Pharma Solutions Limited, Dudley, Cramlington, Northumberland NE23 7QG, UK
dSchool of Chemical and Process Engineering and School of Chemistry, University of Leeds, Leeds, LS2 9JT, UK
eZhejiang Provincial Key Laboratory of Advanced Chemical Engineering Manufacture Technology, College of Chemical and Biological Engineering, Zhejiang University, Hangzhou 310027, P. R. China
fInstitute of Zhejiang University-Quzhou, Quzhou 324000, P. R. China
First published on 23rd October 2023
We present an approach to harnessing the tuneable catalytic properties of complex nanomaterials for continuous flow heterogeneous catalysis by combining them with the scalable and industrially implementable properties of carbon pelleted supports. This approach, in turn, will enable these catalytic materials, which largely currently exist in forms unsuitable for this application (e.g. powders), to be fully integrated into large scale, chemical processes. A composite heterogeneous catalyst consisting of a metal–organic framework-based Lewis acid, MIL-100(Sc), immobilised onto polymer-based spherical activated carbon (PBSAC) support has been developed. The material was characterised by focused ion beam-scanning electron microscopy-energy dispersive X-ray analysis, powder X-ray diffraction, N2 adsorption, thermogravimetric analysis, atomic absorption spectroscopy, light scattering and crush testing with the catalytic activity studied in continuous flow. The mechanically robust spherical geometry makes the composite material ideal for application in packed-bed reactors. The catalyst was observed to operate without any loss in activity at steady state for 9 hours when utilised as a Lewis acid catalyst for the intramolecular cyclisation of (±)-citronellal as a model reaction. This work paves the way for further development into the exploitation of MOF-based continuous flow heterogeneous catalysis.
Heterogeneously catalysed processes are routinely exploited in chemical industry, with 80% of all catalyst-containing chemical processes involving a heterogeneous species.5 However, due to the complexity of designing continuous, multi-phase systems, e.g. obtaining the required mixing of solids and liquids/gases in narrow tubing while avoiding blockages and pressure build-ups caused by catalyst breakdown, the exploitation of heterogeneous catalysis in continuous modes of operation has seen limited but increasing implementation to date.6,7 The translation of heterogeneously catalysed organic transformations to continuous flow therefore offers significant benefits for fine chemical manufacturing.
Progress in the commercial implementation of high-throughput and robust heterogeneously catalysed continuous processes for fine chemical manufacture requires the development of suitable catalyst materials designed across length scales. Both the form (e.g. pellet, powder) and bulk properties (e.g. surface area, immobilisation type) determine the suitability for continuous flow processes.
In their pure form, heterogeneous catalysts typically exist as fine powders and thus their direct application in flow reactors (e.g. packed-bed reactors) may in turn lead to blockages inside the reactor hindering process efficiency, or worse, producing catastrophic pressure build-up. The use of larger-sized shaped supports, such as monoliths, extrudates and porous beads prepared frequently from materials such as alumina, silica, polymers and carbon are used to manage these issues with the active species often anchored to the support.8,9
As well as packing regularly enough to prevent a large pressure drop across the reactor, catalyst supports that are resistant to both crushing and abrasion when inside of the reactor are desirable to avoid breakdown and plug formation. These mechanical considerations are balanced with the requirement of maximising the surface area of the active component of the catalysts and immobilising this species to the support in a manner that ensures sufficient stability for long-term industrial operation (e.g. to prevent leaching or physical detachment over time). Additional consideration must be given to immobilisation approaches as physisorption or the formation of a single covalent bond between the active catalyst and support may not be robust enough for continuous flow operations.10
One promising support material which provides a good balance between macro- and nano-scale properties is polymer-based spherical activated carbon (PBSAC).11 These mechanically strong, commercially available spherical activated carbon pellets have a regular, tuneable size and possess a high, graphitic carbon surface area for catalyst deposition with their successful operation in flow reactors established. Previous research into the use of PBSAC spheres as catalyst supports has primarily involved active species such as metal nanoparticles,12–18 metal oxides19–21 and ionic liquids.22–25 However, composite materials incorporating more complex catalytic nanomaterials, for example metal–organic frameworks (MOFs), is significantly less developed.26,27 MOFs have become attractive candidates as industrial catalysts28 and examples of their application as heterogeneous catalysts in flow reactors, typically packed-bed reactors, have been reported for a range of chemical transformations; such developments have been discussed in detail by Garcia and colleagues.29 Despite initial demonstration of their potential to serve as continuous flow heterogeneous catalysts, however, MOFs typically exist as powders which currently limits their more widespread usage in these reactor platforms.
The MIL-100(M) (M = metal centre) series of MOFs are an isostructural series of large-pore MOFs known to exhibit Lewis acid catalytic activity via metal-containing M3O trimers situated throughout the framework. MOFs of this type have a general stoichiometry of [M3O(BTC)2X], where M is a metal, BTC is benzene-1,3,5-tricarboxylic acid (trimesic acid) and X is a singly charged anion required to balance the positive charge of the framework.30–32 A scandium-based MOF, MIL-100(Sc), has previously been demonstrated to be an active Lewis acid catalyst for intermolecular carbonyl ene and Michael additions.33 MIL-100(Sc) has also been demonstrated to be more catalytically active for such addition reactions than a range of other MOFs on a number of occasions in both batch and continuous flow. Previous studies by Wright et al.33,34 and Čejka et al.35 detail the greater catalytic activity of MIL-100(Sc) when compared to both isostructural MOFs (MIL-100(M), M = Fe, Cr, Al, In) and other MOFs (i.e., MIL-101(Sc), MIL-101(Cr), HKUST-1(Cu), CPO-27(Ni), STA-12(Ni)) in batch. Upon studying MIL-100(Sc) in continuous flow for the carbonation of propylene oxide with CO2, Sanford et al.36 found that this species possessed the highest steady state catalytic activity when compared with a several other catalytically active species (MIL-88D(Sc), MIL-66(Sc), MIL-101(M) (M = Cr, Fe, Sc)) and was also found to exhibit minimal loss in reactivity over a 24 hours continuous operation study. It is important to note that this study focused on testing of powdered MIL-100(Sc) in small scale, continuous flow, with no discussion of routes to scale up. Whilst the formation of composite materials consisting of MIL-100(Fe) and activated carbon has previously been reported,37 the physical form of these materials have always been limited to powders. The formation of MIL-100 MOFs immobilised on macroscopic support materials such as PBSAC spheres is therefore a priority for incorporation into industrially focused, preparative scale, continuous flow reactors.
In this article we report the synthesis, characterisation and initial catalytic activity studies of a novel Lewis acidic heterogeneous catalyst for operation in continuous flow consisting of catalytically active MOF MIL-100(Sc) supported onto PBSAC spheres, termed MIL-100(Sc)@PBSAC. The Lewis acidic catalytic activity of the prepared MIL-100(Sc)@PBSAC composites was studied in continuous flow using the intramolecular cyclisation of (±)-citronellal as a model reaction.
This reaction, when carried out using enantiomerically pure (+)-citronellal, constitutes an important step in the Takasago process for the synthetic production of (−)-menthol, one of the most consumed flavour compounds worldwide with an estimated 30000 metric tonnes of menthol consumed annually.38–40 We show that MIL-100(Sc)@PBSAC composites possesses properties suitable for implementation into industrial flow reactors (e.g. packed bed reactors) for fine chemical synthesis with promising results obtained in preliminary catalytic activity studies.
Before beginning the reaction, toluene was flowed through the solvent-less system at 1 mL min−1 until a continuous liquid phase was observed at the outlet of the reactor and a stable pressure was achieved. The reactor, which was clamped vertically, was heated using an aluminium heating block which was connected to a Eurotherm temperature controller set to 110 °C. A solution of (±)-citronellal (0.43 M in toluene, n-decane internal standard) was pumped from bottom to top for ideal distribution throughout the packed-bed. The resultant outlet stream was analysed offline by gas chromatography. For the preparation of GC samples, 10 μL of the outlet stream was diluted to a total volume of 1 mL with toluene.
Thermogravimetric analysis (TGA) was carried out on a Shimadzu TGA-50. A typical analysis involved heating approximately 10 mg of the sample from 20 °C to 900 °C at 10 °C min−1 in flowing air (50 mL min−1).
Atomic absorption spectroscopy (AAS) was carried out using an Agilent 200 series AA system. Samples were prepared for analysis by heating in air a known amount at 600 °C for 90 minutes with the resultant white solid dissolved in nitric acid (10 mL, 67%). Following dissolution the sample was then diluted to a known volume (30 ppm) for analysis.
N2 adsorption analysis was carried out at −196 °C using a Micrometrics Tristar 3000. Samples (≈50 mg) were activated prior to analysis by heating at 150 °C overnight under a flow of N2. Brunauer–Emmett–Teller (BET) surface areas were calculated using the BETSI method.42 Pore volumes were obtained P/Po = 0.99. Micropore volumes were extracted from t-plots.
Gas chromatography (GC) analysis was carried out on a Hewlett Packard HP 6890 series GC system using a DB-624 column (length: 30 m, diameter: 0.25 m, film thickness: 1.40 μm) and FID detector at 300 °C. See ESI section 1.2† for specific method information.
PBSAC support particle size distributions were obtained using a Malvern Mastersizer 3000 laser diffraction system. PBSAC spheres, which were stirred in water using the Hydro MV automated wet dispersion unit with a stirring rate of 3500 rpm, were added until the laser obscuration reached between 10–20%.
Crush testing was done using an Instron 5566 according to a modified version of the ASTM D-4179 standard test for single pellet crush strength. Samples were heated to 250 °C under dynamic vacuum for 3 hours to remove water and then stored under nitrogen and in a desiccator until analysis. For measurements, increasing force at a uniform rate of 0.05 N s−1 was applied until crushing of the particle occurred. For each sample, 50 particles were crushed.
Focused ion beam-scanning electron microscopy (FIB-SEM) and energy dispersive X-ray (EDX) analysis of materials was carried out on an FEI Helios G4 CX DualBeam. Prior to imaging, 20 nm of carbon coating was evaporated onto the sample surface using a Quorum Q150TE coater to reduce charging. Images were collected using a standard ETD (Everhart–Thornley detector) in secondary electron mode or a CBS (circular backscattered electron detector) detector. The typical voltage used was 5 or 10 kV. EDX analysis was carried out using an Oxford instruments AZtec energy EDX system with a 150 mm X-Max SDD detector. The Ga source for the FIB was operated at 30 kV.
The stoichiometry of MIL-100(Sc) in this work was determined to be [Sc3O(BTC)1.45OH2.65] by carrying out TGA analysis on a powdered MIL-100(Sc) sample and thus for catalyst synthesis reagent amounts which gave a maximum MIL-100(Sc) loading of 11.87% w/w (a scandium loading of 3.23% w/w) onto PBSAC spheres was selected (Table 1). This loading value was selected as it provides a balance between minimising cost in the initial catalyst development stage whilst also ensuring sufficient catalytic activity.
Molar ratio (PBSAC:M:L:DMF)a | Resultant maximum possible scandium loading (% w/w) | Resultant maximum possible MIL-100(Sc) loading (% w/w) |
---|---|---|
a Where PBSAC, M, L and DMF is the amount of PBSAC spheres, scandium nitrate hydrate, benzene-1,3,5-tricarboxylic acid and DMF respectively in moles. For molar ratio calculations it was assumed that PBSAC spheres are composed of 100% carbon, a molecular weight of 12.01 g mol−1. | ||
212:2:1:600 | 3.23 | 11.87 |
Under the synthetic conditions employed for the preparation of MIL-100(Sc)@PBSAC composites, the formation of loose, powdered MIL-100(Sc) independent of the PBSAC as a white solid was observed in the reaction vessel. This powder was confirmed as crystalline MIL-100(Sc) by powder X-ray diffraction (ESI section 1.4†) suggesting that not all MIL-100(Sc) that formed was immobilised onto PBSAC spheres. Similarly to previous observations with other MOF@AC composite materials,41 the appearance of MIL-100(Sc)@PBSAC was seemingly unchanged from the as received PBSAC spheres (Fig. 1a). Additionally, a small amount of material was lost from the PBSAC in the form of black powder owing to impact with the stirrer bar inside of the reaction vessel over time. After synthesis, the material was activated by stirring in methanol for 72 hours at 40 °C to replace residual solvent material present inside of the pores of the framework and then dried at 60 °C under vacuum.
The surface structure and location of MIL-100(Sc) on PBSAC spheres was studied using scanning electron microscopy and energy dispersive X-ray analysis (SEM-EDX) (Fig. 1b–f). Although not visible to the naked eye, imperfections such as scratches and cracks (≈3 μm in width) are situated throughout the outer surface of unfunctionalised PBSAC spheres (see ESI section 1.5†). MIL-100(Sc) appears to crystallise inside these cracks preferentially (Fig. 1b–d) and thus exploitation of this feature may be one approach to controlling the loading of MOFs on PBSAC spheres.
EDX mapping of the surface of MIL-100(Sc)@PBSAC suggests that the majority of MIL-100(Sc) is present within the cracks situated as indicated by the counts of the scandium Kα line scan across the surface and a crack (Fig. 1e and f).
To gain insight into both the depth of the cracks on the surface of the spheres and how far down MIL-100(Sc) resides into these cracks, FIB-SEM-EDX was used. A section of the surface of a MIL-100(Sc)@PBSAC bead was etched away to a depth of 10 μm and analysed by EDX analysis (Fig. 2a–d). This analysis revealed the cracks penetrate further than 10 μm into the surface of the PBSAC spheres, but that a majority of the MIL-100(Sc) that is immobilised in these cracks resides near the surface (approximately 2.5 μm from the surface).
The presence of crystalline MIL-100(Sc) immobilised onto the PBSAC spheres was confirmed using powder X-ray diffraction (Fig. 3a and b). Despite significant diffuse background scattering in the powder pattern of MIL-100(Sc)@PBSAC as a result of the amorphous phases present in the activated carbon support,41,43 there are visible peaks at 2θ = 3–4.5, 9.5–11 and 17–20 present corresponding to the presence of crystalline MIL-100(Sc) as indicated by comparison with the underlying simulated pattern of MIL-100(Sc) (calculated by adjusting the unit cell parameter (a) of MIL-100(Cr), as reported previously44) and reflux prepared powdered MIL-100(Sc).30,33 This pattern confirms that crystalline MIL-100(Sc) was incorporated onto the PBSAC spheres.
Upon immobilisation of MIL-100(Sc) onto PBSAC spheres, there is a decrease in the total pore volume of PBSAC from 1.23 cm3 g−1 to 1.07 cm3 g−1 suggesting that MIL-100(Sc) is partially occupying the pores of PBSAC spheres (Table 2). There is also no significant difference in the micropore volume of MIL-100(Sc)@PBSAC (0.39 cm3 g−1) compared to unfunctionalised PBSAC spheres (0.41 cm3 g−1). Fig. 3d shows the BJH desorption differential pore volumes of PBSAC, MIL-100(Sc)@PBSAC and MIL-100(Sc) in the range of 0–50 nm. This visualisation illustrates that there is a decrease in the pore volume of MIL-100(Sc)@PBSAC composites compared to unfunctionalised PBSAC spheres.
Insight into the thermal stability of the materials and the loading of MIL-100(Sc) on PBSAC spheres was obtained using thermogravimetric analysis (TGA) (Fig. 4). There are three characteristic mass changes in the TGA profiles of MIL-100 MOFs: at 0–100 °C is the removal of free solvent present in the pores of the framework, 100–350 °C shows loss of more tightly bound solvent to the metal centres throughout the framework and finally at ≈400 °C the breakdown of the MOF structure occurs.30 When analysed in air, the residual mass in the TGA profile of powdered MIL-100(Sc) corresponds to the mass of Sc2O3 that was formed following framework decomposition. By comparing the mass of residual scandium present after framework decomposition to the mass of MIL-100(Sc) present after solvent removal but before framework decomposition (at ≈400 °C), the stoichiometry of MIL-100(Sc) was inferred.
Fig. 4 TGA profiles of PBSAC (yellow), MIL-100(Sc)@PBSAC (green) and MIL-100(Sc) (blue) in flowing air. |
When prepared by reflux, powdered MIL-100(Sc) possesses a scandium wt% of 27.2%, as inferred from the TGA data. This scandium wt% value may correspond to a ‘dry’ (i.e. following solvent removal) stoichiometry of [Sc3O(BTC)1.45OH2.65] where it is assumed that the anion used to balance the charge of the framework is OH− (see ESI section 1.7† for calculation). Upon the assumption that this is also the formula of MIL-100(Sc) that is incorporated onto PBSAC spheres, then full incorporation of the scandium used in the synthesis of MIL-100(Sc)@PBSAC composites gives a 11.87% MIL-100(Sc) loading (a scandium loading of 3.23% w/w).
By carrying out an analogous calculation with the mass values obtained in the TGA profile of MIL-100(Sc)@PBSAC composites but by adjusting the residual mass by subtracting the residual mass in the TGA profile of PBSAC spheres, the MIL-100(Sc) loading was calculated to be 6.42 ± 1.93% w/w (a scandium loading of 1.75 ± 0.52% w/w). The loading value obtained by carrying out these calculations was also similar in value to what was obtained with atomic absorption spectroscopy (AAS) where a MIL-100(Sc) loading value of 5.71 ± 0.93% w/w (a scandium loading of 1.55 ± 0.25% w/w) onto PBSAC spheres was measured. The loading values that were calculated were lower than the maximum value based on the mass of Sc used in the preparation (11.87% w/w MIL-100(Sc) loading), which is in keeping with the observed formation of loose powdered MIL-100(Sc) in the reaction vessel alongside MIL-100(Sc)@PBSAC spheres and thus was not included in loading calculations.
In the TGA profile of the MIL-100(Sc)@PBSAC composite (Fig. 4), the material exhibits a steady decrease in mass of approximately 5% (corresponding to the loss of material bound to the Sc3+ sites) before framework decomposition occurred at ≈380 °C. The composite MIL-100(Sc)@PBSAC was found to be less thermally stable than unfunctionalised PBSAC spheres where thermal decomposition occurred at ≈550 °C; with the thermal decomposition temperature being more similar in value to that of powdered MIL-100(Sc) where framework decomposition begins to occur at ≈380 °C. Upon incorporation into PBSAC spheres, the thermal stability of MIL-100(Sc) was shown not to improve, despite previous reports of enhanced MOF stability upon incorporation onto AC substrates.37 Inspection of the derivative weight loss curves of MIL-100(Sc) and MIL-100(Sc)@PBSAC (Fig. SI13†) shows that material decomposition occurs at a very similar temperature (maximum rate of weight loss at ≈520 °C).
As well as the crush strength, the particle size of PBSAC spheres was determined in order to calculate reactor tube diameter (Dt) to particle diameter (Dp) ratio (Dt/Dp ratio) as this may have implications on the uniformity of liquid flow through the column. Generally speaking, a Dt/Dp ratio of ≥15 is desirable to minimise flow maldistribution across the reactor.48 With a D10, D50 and D90 (corresponding to the diameter below which 10%, 50% or 90% of particles are smaller than respectively) of 359 μm, 465 μm and 602 μm respectively (see ESI section 1.9† for volume distribution graph), 1/2′′ tubing with an internal diameter of 3/8′′ was selected for the packed bed reactor. This ensures uniform flow across the catalyst bed upon operation in continuous flow as the Dt/Dp ratio varied from approximately 16–27 (between the D10 to D90 value range) (Table 3).
Due to the industrial significance of this reaction, it is frequently used to quantify and compare the Lewis acidic catalytic activity of novel catalysts, both homogeneous and heterogeneous,50 with the use of the more economical racemic equivalent, (±)-citronellal, often preferred. When studying this reaction using a novel Lewis acid catalyst, which is most frequently done in a batch mode of operation, important metrics include the rate of the reaction as well as the selectivity towards the formation of (±)-isopulegols and diastereoselectivity towards (±)-isopulegol formation.
To date, there are examples regarding the implementation of this reaction into continuous flow systems,51–58 but none (to the best of the authors knowledge) that employ a MOF-based catalyst in this mode of operation. Many examples still exist regarding the catalysis of this reaction by MOFs in batch and discontinuous flow, Table 5 summarises some of the most popular examples to date. For this reason, and due to the industrial importance of this reaction we therefore sought to explore the catalytic activity of novel MIL-100(Sc)@PBSAC heterogeneous catalyst composites in continuous flow.
A packed-bed reactor was filled with a combination of MIL-100(Sc)@PBSAC composite spheres and an inert packing material (500 μm glass beads) and heated to 110 °C. A solution of (±)-citronellal (0.43 M) was flowed through at 0.25 mL min−1 (Fig. 5a). The catalytic activity, selectivity and efficiency was studied over the course of 9 hours time-on-stream (Fig. 5b–d). The average results of the 9 hours time-on-stream are summarised in Table 4 (see ESI section 2† for calculations of reaction metrics).
Conversion (%) | Yield of (±)-isopulegols (%) | Selectivity to (±)-isopulegols (%) | Selectivity to (±)-isopulegol (%) | Productivitya (g h−1) | TON after 9 hoursb | TOFc (h−1) |
---|---|---|---|---|---|---|
a Productivity represents the average amount of (±)-isopulegols formed, in g, per hour over the 9 hours on stream. b TON after 9 hours = amount of (±)-isopulegols formed after 9 hours (in moles)/amount of catalyst (in moles). c TOF (h−1) = TON per hour/time (in hours) for the 9 hours time-on-stream. Calculation of TON and TOF assumed that all scandium atoms in the MIL-100(Sc) framework participated in catalysis. | ||||||
72.9 ± 5.2 | 64.4 ± 1.3 | 88.8 ± 6.5 | 66.0 ± 0.6 | 0.64 ± 0.01 | 95.6 | 10.6 ± 0.2 |
Based on the liquid flow rate (0.25 mL min−1) and volume of the packed reactor (8.5 mL), the residence time was calculated to be 34 minutes. Sampling was carried out using offline gas chromatography, with an initial spike in the conversion of (±)-citronellal (86%) after one hour observed when compared to the steady conversion value that was measured over the next 8 hours time-on-stream between 69–76% (Fig. 5b). Conversion was determined by comparison of the initial (±)-citronellal concentration with the concentration that was present upon exiting the reactor. Thus, this initial spike may be indicative of phenomena such as (±)-citronellal adsorption onto the catalyst or the initial mass transfer of (±)-citronellal molecules into the pore network of the MIL-100(Sc)@PBSAC composites which, at the start of the reaction, were only filled with toluene and unoccupied by reactant molecules.
The catalytic activity (i.e. the amount of (±)-citronellal converted per gram of catalyst per hour) was measured over the course of the 9 hours time-on-stream and compared with the current literature (Table 5, column 5). MIL-100(Sc)@PBSAC composites were found to be the second most active MOF-based species to catalyse this reaction (72.9 ± 5.2 mmol gcat−1 h−1) to date after superacidic MOF-808-2.5SO4 (83.1 mmol gcat−1 h−1),64 with an Sn-β zeolite catalyst found overall to be the most active (341.2 mmol gcat−1 h−1). In some cases, the catalytic activity of MIL-100(Sc)@PBSAC composites was found to be two orders of magnitude greater than other species (i.e. Cu3(BTC)2, MIL-100(Fe), MIL-101(Cr), Pd@MIL-100(Cr), Zr(Ti)-NDC).
Catalyst | Mode | Temperature (°C) | Solvent | Activitya (mmol gcat−1 h−1) | Selectivity to (±)-isopulegols (%) | Selectivity to (±)-isopulegol (%) | Ref. |
---|---|---|---|---|---|---|---|
a Data for other catalysts taken from work carried out by Wade et al.59 Calculated as mmol of citronellal converted per gram of catalyst (MIL-100(Sc)) per hour. b Coincidentally conversion and activity values were identical for MIL-100(Sc)@PBSAC composites. c UiO-66 synthesised with different equivalents of TFA. d For hydrated and dehydrated UiO-66 respectively. e Obtained following treatment with SO4: MOF-808-2.5SO4. f Decreased with increasing acid activation. g PNNNP-Pd pincer complexes immobilised onto MFU-4l-OH. h Carried out in microwave oven. i Zeolite. j Mesoporous silicate. | |||||||
MIL-100(Sc)@PBSAC | Flow | 110 | Toluene | 72.9 ± 5.2b | 88.8 ± 6.5 | 66.0 ± 0.6 | (This work) |
UiO-66-NO2 | Batch | 100 | Toluene | 4.9 | — | 81 | 61 |
UiO-66 | Batch | 110 | Toluene | — | — | 75–77c | 62 |
(De)hydrated UiO-66 | Batch | 80 | Cyclohexane | 0.4 and 1.3d | — | 75 and 86d | 63 |
MOF-808 | Batch | 60 | Toluene | 83.1e | — | 55–85f | 64 |
Cu3(BTC)2 | Batch | 110 | Toluene | 0.6 | >99 | 65–69 | 65 |
MIL-100(Fe) | Batch | 50 | Acetone | 0.2 | — | — | 66 |
MIL-101(Cr) | Batch | 80 | Cyclohexane | 0.6 | >99 | 74 | 60 |
Pd@MIL-101(Cr) | Batch | 80 | Cyclohexane | 0.9 | >99 | 73 | 60 |
PdBF4g | Batch | 100 | Toluene | 4.1–12.2g | — | 65 | 59 |
Zr(Ti)-NDC | Batch | 150h | Toluene | 0.6 | 99 | 76 | 67 |
Sn-βi | Flow | 80 | Acetonitrile | 341.2 | 99 | 83 | 55 |
H-βi | Batch | 80 | Cyclohexane | — | >99 | 75 | 68 |
Ir/H-βi | Batch | 80 | Cyclohexane | — | >99 | 75 | 68 |
Zr-TUD-1j | Batch | 80 | Toluene | — | >99 | 65 | 69 |
For the duration of the experiment there was a stable yield (62–67%) towards the formation of (±)-isopulegols (Fig. 5b and c) meaning that, on average, 89% of the (±)-citronellal that was converted (conversion measured as difference in (±)-citronellal concentration at start and outlet of reactor) was forming (±)-isopulegols. The diastereoselectivity of the reaction, that is, the selectivity towards the formation of (±)-isopulegol compared to other (±)-isopulegols, also remained very consistent at between 65–67% over the 9 hours-on-stream (Fig. 5b and c). This value is in a similar range with what has previously been obtained with other powdered, unsupported MOF catalysts in batch (Table 5, column 8). The fact that the diastereoselectivity remained constant over the course of the 9 hours means that consistent amounts of (±)-isopulegol were reliably synthesised inviting potential for the introduction of downstream reaction modules to the system (e.g. tandem hydrogenation to produce (±)-menthol) which is enabled intrinsically by the continuous mode of operation used.
A total amount of 5.7 g of (±)-isopulegols were produced with an average productivity of 0.64 g h−1 (Table 4 and Fig. 5d); such numbers translate to a cumulative turnover number (TON) of 92.9 and turnover frequency (TOF) of 10.3 h−1.
Over the 9 hours on stream, the reaction ran smoothly with no reactor blockages or downtime. Additionally, no physical destruction of the catalyst (e.g. attrition, crushing) was observed following visual inspection after use. These positive results briefly showcase the high potential and robustness of this support material for use in continuous systems in the future. The consistent rate of reaction over 9 hours on stream as indicated by the consistent TON values indicated minimal loss of catalyst from the reactor. However, after longer reaction times (26 hours) some loss of scandium from the support (7.5–13.6%) was observed (ESI section 2.1.1†) with the conversion also decreasing to 41% while SEM examination of the catalyst after 26 hours of reaction showed no observable changes (ESI section 2.1.2†).
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3nr03634k |
This journal is © The Royal Society of Chemistry 2023 |